Blue, Yellow, and Red Carbon Dots from Aromatic Precursors for Light-Emitting Diodes

In this work, multicolor fluorescent carbon dots with red (R-CDs), yellow (Y-CDs), and blue (B-CDs) emissions were prepared by choosing proper aromatic precursors with different amounts of benzene rings through a simple solvothermal method. The characterization showed that the prepared carbon dots were spherical with a size under 10 nm, rich surface functional groups, and good stability. The emission wavelengths were located at 440, 530, and 580 nm under the excitation of 370 nm. The relative fluorescence quantum yield (QY) of R-CDs, Y-CDs, and B-CDs was 11%, 59%, and 33%, respectively. The related characterization demonstrated that the redshift in the photoluminescence was caused by the synergistic effect of the increasing graphitic nitrogen content, quantum size effect and surface oxidation state. By mixing the three prepared CDs into a PVA matrix, the transparent and flexible films produced relucent blue, yellow, and red emissions under 365 nm UV light, and solid-state quenching was effectively avoided. LEDs were fabricated by using B-CDs, Y-CDs, and R-CDs/PVA with a semiconductor chip. These CDs-based LEDs produced bright blue, yellow, and red light with CIE color coordinates of (0.16, 0.02), (0.38, 0.58), and (0.50, 0.49) were successfully manufactured utilizing the prepared blue, yellow and red multicolor carbon dots as the solid luminescent materials. The results showed that the synthesized CDs can be potentially applied in multi-color monitors as a promising candidate for light-emitting diodes (LEDs). This work blazes a novel trail for the controllable preparation of multicolor fluorescent carbon dots.

The tunable and multicolor PL property is so fascinating that researchers are making great efforts to synthesize, modify, and functionalize CDs in order to regulate and control the emission of CDs. The multicolor emission can be adjusted by the excitation of the wavelength, pH, the concentration, solvent used, carbon source, reaction condition, separation, and pressure [11,12]. Reaction conditions play a vital role in the synthesis of MCDs. Reaction conditions include changing the response temperature [13], time [14], reactant ratio [11], reaction solvent type [15,16], and pH [17], or using machine learning assistance [18]. Among them, the reaction temperature influences the carbonization of carbon resources, then affects the degree of graphitization [1,13]. During synthesis, the reaction time influences the degree of the completion of MCDs, then affects the surface oxidation and size of the CDs [14]. The reaction solvent will control the degree of carbonization and dehydration in the carbon precursors, and then affects the size of the sp 2 -conjugated domains [16]. The According to the photoluminescence mechanism of CDs, the conjugation length and the sp 2 domain size influence the emission. Therefore, considering the conjugation structure of benzene ring, we choose three typical aromatic precursors (aniline, 1,8diaminonaphthalene, and [1,1 -binaphthalene]-2,2 -diamine) with different benzene rings with different conjugation degrees in order to synthesize CDs. The use of o-phenylenediamine was favorable to form conjugated sp 2 domains and nitrogen-containing groups in the CD formation process.
In order to explore the influence of precursors on the fluorescence emission of the MCDs, three CDs were selected as typical samples in order to investigate the principle. According to the particular emission colors, they were named B-CDs, Y-CDs, and R-CDs, re-spectively. MCDs were obtained under the following conditions: o-phenylenediamine/[1,1binaphthalene]-2,2 -diamine = 1 at 180 • C for B-CDs, o-phenylenediamine/aniline = 1 at 180 • C for Y-CDs, and o-phenylenediamin/1,8-diaminonaphthalene = 1 at 180 • C for R-CDs, respectively.
The morphology and particle size of B-CDs, Y-CDs, and R-CDs were investigated by HRTEM, the results of which are shown in Figure 1. The three kinds of CDs were spherical and well dispersed, without obvious aggregation. The calculated average sizes of the B-CDs, Y-CDs, and R-CDs were 1.97 ± 0.24, 2.19 ± 0.32, and 2.51 ± 0.28 nm, respectively, and had a relatively uniform size distribution.
Molecules 2023, 28, x FOR PEER REVIEW 3 of 12 According to the particular emission colors, they were named B-CDs, Y-CDs, and R-CDs, respectively. MCDs were obtained under the following conditions: o-phenylenediamine/[1,1′-binaphthalene]-2,2′-diamine = 1 at 180 °C for B-CDs, o-phenylenediamine/aniline = 1 at 180 °C for Y-CDs, and o-phenylenediamin/1,8-diaminonaphthalene = 1 at 180 °C for R-CDs, respectively. The morphology and particle size of B-CDs, Y-CDs, and R-CDs were investigated by HRTEM, the results of which are shown in Figure 1. The three kinds of CDs were spherical and well dispersed, without obvious aggregation. The calculated average sizes of the B-CDs, Y-CDs, and R-CDs were 1.97 ± 0.24, 2.19 ± 0.32, and 2.51 ± 0.28 nm, respectively, and had a relatively uniform size distribution. Fourier-transform infrared (FTIR), Raman, X-ray powder diffraction (XRD), and Xray photoemission spectroscopy spectra (XPS) analyses were also carried out to interpret the chemical compositions and surface functional groups of the prepared CDs.
As shown in Figure 2a, compared with B-CDs, the XRD pattern of the Y-CDs and R-CDs expressed a minor sharp peak at 26.6°, which was due to the graphite structure with a layer spacing (002) of 0.41 and 0.34 nm [29]. The 26.6° peak was defined as the characteristic diffraction peak (002) of graphite. Its existence indicates the interlayer stacking between the CDs, which is like that of graphite (≈0.35 nm). This suggests that a similar accumulation (0.35 nm) of highly conjugated sp 2 domains is dominant in CDs. At the edge of the CDs, the sp 3 carbon or functional groups increase the inter-layer distance. The R-CD peak at 26.6° was the highest, thus predicting the greatest extent of graphitization; this suggested that R-CDs had a greater effective conjugation length than B-CDs and Y-CDs [30].  Figure S1 shows the Raman spectra of the prepared MCDs, which exhibited two peaks at 1,354 cm −1 and 1,581 cm −1 , corresponding to the disordered (D band) and graphite (G band) of the carbon material. As we know, the ratio of ID/IG equals the ratio of sp 3 /sp 2 Fourier-transform infrared (FTIR), Raman, X-ray powder diffraction (XRD), and X-ray photoemission spectroscopy spectra (XPS) analyses were also carried out to interpret the chemical compositions and surface functional groups of the prepared CDs.
As shown in Figure 2a, compared with B-CDs, the XRD pattern of the Y-CDs and R-CDs expressed a minor sharp peak at 26.6 • , which was due to the graphite structure with a layer spacing (002) of 0.41 and 0.34 nm [29]. The 26.6 • peak was defined as the characteristic diffraction peak (002) of graphite. Its existence indicates the interlayer stacking between the CDs, which is like that of graphite (≈0.35 nm). This suggests that a similar accumulation (0.35 nm) of highly conjugated sp 2 domains is dominant in CDs. At the edge of the CDs, the sp 3 carbon or functional groups increase the inter-layer distance. The R-CD peak at 26.6 • was the highest, thus predicting the greatest extent of graphitization; this suggested that R-CDs had a greater effective conjugation length than B-CDs and Y-CDs [30].
The morphology and particle size of B-CDs, Y-CDs, and R-CDs were investigated by HRTEM, the results of which are shown in Figure 1. The three kinds of CDs were spherical and well dispersed, without obvious aggregation. The calculated average sizes of the B-CDs, Y-CDs, and R-CDs were 1.97 ± 0.24, 2.19 ± 0.32, and 2.51 ± 0.28 nm, respectively, and had a relatively uniform size distribution. Fourier-transform infrared (FTIR), Raman, X-ray powder diffraction (XRD), and Xray photoemission spectroscopy spectra (XPS) analyses were also carried out to interpret the chemical compositions and surface functional groups of the prepared CDs.
As shown in Figure 2a, compared with B-CDs, the XRD pattern of the Y-CDs and R-CDs expressed a minor sharp peak at 26.6°, which was due to the graphite structure with a layer spacing (002) of 0.41 and 0.34 nm [29]. The 26.6° peak was defined as the characteristic diffraction peak (002) of graphite. Its existence indicates the interlayer stacking between the CDs, which is like that of graphite (≈0.35 nm). This suggests that a similar accumulation (0.35 nm) of highly conjugated sp 2 domains is dominant in CDs. At the edge of the CDs, the sp 3 carbon or functional groups increase the inter-layer distance. The R-CD peak at 26.6° was the highest, thus predicting the greatest extent of graphitization; this suggested that R-CDs had a greater effective conjugation length than B-CDs and Y-CDs [30].  Figure S1 shows the Raman spectra of the prepared MCDs, which exhibited two peaks at 1,354 cm −1 and 1,581 cm −1 , corresponding to the disordered (D band) and graphite (G band) of the carbon material. As we know, the ratio of ID/IG equals the ratio of sp 3 /sp 2  Figure S1 shows the Raman spectra of the prepared MCDs, which exhibited two peaks at 1354 cm −1 and 1581 cm −1 , corresponding to the disordered (D band) and graphite (G band) of the carbon material. As we know, the ratio of I D /I G equals the ratio of sp 3 /sp 2 carbon, which represents the extent of graphite. The calculated ratio of I D /I G was 0.91, 0.66, and 1.30 for B-, Y-, and R-CDs, respectively. A relatively lower I D /I G for the B-CDs and Y-CDs indicated the much higher disorder degree of CDs.
In order to further explore the chemical structure of MCDs, the FTIR spectra of MCDs were tested, as shown in Figure 2b the board peak located at 3420 cm −1 was assigned to the N-H/O-H groups, the peak located at 2990 cm −1 was assigned to the -CH 2 group, and the stretching vibrations for -C-C, -C=C, and C=O were located at 1340, 1500, and 1685 cm −1 , respectively. These results indicated that the conjugated aromatic structure of the carbon core and the surface functional groups containing N and O (-COOH, -OH, -NH 2 ) were incorporated successfully. At the same time, the gradually broadened C=O peak from the B-CDs, Y-CDs to R-CDs reflected the increase in carboxyl groups on the surface of MCDs.
To further determine the surface state and chemical composition of MCDs, XPS (X-ray photoelectron spectroscopy) was used to characterize the MCDs. As is evident in Figure S2, the full XPS spectra of MCDs showed three predominant peaks at 284.5 eV, 400 eV, and 532 eV, indicating the existence of C 1s , N 1s , and O 1s , respectively.
Taking the high-resolution XPS spectrum of the R-CDs as an example, the highresolution C 1s band (Figure 3a Table S1. carbon, which represents the extent of graphite. The calculated ratio of ID/IG was 0.91, 0.66, and 1.30 for B-, Y-, and R-CDs, respectively. A relatively lower ID/IG for the B-CDs and Y-CDs indicated the much higher disorder degree of CDs. In order to further explore the chemical structure of MCDs, the FTIR spectra of MCDs were tested, as shown in Figure 2b the board peak located at 3,420 cm −1 was assigned to the N-H/O-H groups, the peak located at 2,990 cm −1 was assigned to the -CH2 group, and the stretching vibrations for -C-C, -C=C, and C=O were located at 1,340, 1,500, and 1,685 cm −1 , respectively. These results indicated that the conjugated aromatic structure of the carbon core and the surface functional groups containing N and O (-COOH, -OH, -NH2) were incorporated successfully. At the same time, the gradually broadened C=O peak from the B-CDs, Y-CDs to R-CDs reflected the increase in carboxyl groups on the surface of MCDs.
To further determine the surface state and chemical composition of MCDs, XPS (Xray photoelectron spectroscopy) was used to characterize the MCDs. As is evident in Figure S2, the full XPS spectra of MCDs showed three predominant peaks at 284.5 eV, 400 eV, and 532 eV, indicating the existence of C1s, N1s, and O1s, respectively.
Taking the high-resolution XPS spectrum of the R-CDs as an example, the high-resolution C1s band (Figure 3a Table S1. With the increased number of benzene rings in the carbon precursors, the ratio of C to N changed from 2.41, 1.77 to 1.90, while the ratio of O/C increased from 0.29, 0.40 to 0.42 for B-CDs, Y-CDs, and R-CDs, respectively, which indicated that the increase in the oxygen amounts was caused by the presence of carboxylic groups [27]. The content of the With the increased number of benzene rings in the carbon precursors, the ratio of C to N changed from 2.41, 1.77 to 1.90, while the ratio of O/C increased from 0.29, 0.40 to 0.42 for B-CDs, Y-CDs, and R-CDs, respectively, which indicated that the increase in the oxygen amounts was caused by the presence of carboxylic groups [27]. The content of the carboxyl group significantly increased from B-CDs, Y-CDs, to R-CDs, which agreed with the FTIR result. When there was more surface oxidation present on the MCDs, there were more surface defects. Meanwhile, the content of the graphitic N (C-N-C) group was increased from the B-CDs and Y-CDs to R-CDs, according to the XPS results. The existence of more C-N-C groups revealed that much more o-phenylenediamine was integrated with 1,8-diaminonaphthalene; this formed larger conjugate sp 2 domains, as well as the effective conjugation length, thus resulting in the redshift in the emission. Figure 4a shows the UV-vis absorption spectrum of the prepared MCDs. B-CDs exhibited a strong absorption band at 360 nm, which was always ascribed to the n-π* transitions, conjugated to C=O and C=N. For Y-CDs, an absorption band was observed at 430 nm. The absorption peak of the R-CDs appeared at 500 nm. These peaks were considered as n-π* transitions in the aromatic sp 2 system containing C=O and C=N bonds.

Spectral Properties of the Prepared CDs
Molecules 2023, 28, x FOR PEER REVIEW 5 of 12 carboxyl group significantly increased from B-CDs, Y-CDs, to R-CDs, which agreed with the FTIR result. When there was more surface oxidation present on the MCDs, there were more surface defects. Meanwhile, the content of the graphitic N (C-N-C) group was increased from the B-CDs and Y-CDs to R-CDs, according to the XPS results. The existence of more C-N-C groups revealed that much more o-phenylenediamine was integrated with 1,8-diaminonaphthalene; this formed larger conjugate sp 2 domains, as well as the effective conjugation length, thus resulting in the redshift in the emission. Figure 4a shows the UV-vis absorption spectrum of the prepared MCDs. B-CDs exhibited a strong absorption band at 360 nm, which was always ascribed to the n-π* transitions, conjugated to C=O and C=N. For Y-CDs, an absorption band was observed at 430 nm. The absorption peak of the R-CDs appeared at 500 nm. These peaks were considered as n-π* transitions in the aromatic sp 2 system containing C=O and C=N bonds. As displayed in Figure 5, the fluorescence emission spectra of B-, Y-, and R-CDs at different excitation wavelengths were measured. The emission wavelength of the Y-CDs was dependent on the excitation wavelength. When the excitation wavelength of Y-CDs transformed from 410 to 500 nm, the emission wavelength gradually shifted from 520 to 555 nm. However, the emission peak of B-CDs was mainly 410 nm in the excitation wavelength range of 340~400 nm, indicating that it was an excitation-independent emission. In the excitation wavelength range of 430~540 nm, the emission range of R-CDs was longer, and the maximum emission peak was 580 nm. Different from Y-CDs, both B-CDs and R-CDs displayed excitation-independent emission behavior, which probably depended on their homogeneous surface states. Meanwhile, the excitation-dependent FL behavior was caused by the doping of graphitic nitrogen.  As displayed in Figure 5, the fluorescence emission spectra of B-, Y-, and R-CDs at different excitation wavelengths were measured. The emission wavelength of the Y-CDs was dependent on the excitation wavelength. When the excitation wavelength of Y-CDs transformed from 410 to 500 nm, the emission wavelength gradually shifted from 520 to 555 nm. However, the emission peak of B-CDs was mainly 410 nm in the excitation wavelength range of 340~400 nm, indicating that it was an excitation-independent emission. In the excitation wavelength range of 430~540 nm, the emission range of R-CDs was longer, and the maximum emission peak was 580 nm. Different from Y-CDs, both B-CDs and R-CDs displayed excitation-independent emission behavior, which probably depended on their homogeneous surface states. Meanwhile, the excitation-dependent FL behavior was caused by the doping of graphitic nitrogen. carboxyl group significantly increased from B-CDs, Y-CDs, to R-CDs, which agreed with the FTIR result. When there was more surface oxidation present on the MCDs, there were more surface defects.

Spectral Properties of the Prepared CDs
Meanwhile, the content of the graphitic N (C-N-C) group was increased from the B-CDs and Y-CDs to R-CDs, according to the XPS results. The existence of more C-N-C groups revealed that much more o-phenylenediamine was integrated with 1,8-diaminonaphthalene; this formed larger conjugate sp 2 domains, as well as the effective conjugation length, thus resulting in the redshift in the emission. Figure 4a shows the UV-vis absorption spectrum of the prepared MCDs. B-CDs exhibited a strong absorption band at 360 nm, which was always ascribed to the n-π* transitions, conjugated to C=O and C=N. For Y-CDs, an absorption band was observed at 430 nm. The absorption peak of the R-CDs appeared at 500 nm. These peaks were considered as n-π* transitions in the aromatic sp 2 system containing C=O and C=N bonds. As displayed in Figure 5, the fluorescence emission spectra of B-, Y-, and R-CDs at different excitation wavelengths were measured. The emission wavelength of the Y-CDs was dependent on the excitation wavelength. When the excitation wavelength of Y-CDs transformed from 410 to 500 nm, the emission wavelength gradually shifted from 520 to 555 nm. However, the emission peak of B-CDs was mainly 410 nm in the excitation wavelength range of 340~400 nm, indicating that it was an excitation-independent emission. In the excitation wavelength range of 430~540 nm, the emission range of R-CDs was longer, and the maximum emission peak was 580 nm. Different from Y-CDs, both B-CDs and R-CDs displayed excitation-independent emission behavior, which probably depended on their homogeneous surface states. Meanwhile, the excitation-dependent FL behavior was caused by the doping of graphitic nitrogen.  The optimal excitation and emission wavelength of B-, Y-, and R-CDs (Figure 4b) were 370/440 nm, 430/530 nm, and 520/580 nm, respectively. The optimal excitation wave-lengths of these three CDs were basically consistent with their corresponding absorption bands, indicating that the emission mainly acted on the absorption bands from the n-π* transition of the C=O and C=N bonds of the aromatic sp 2 system.

Spectral Properties of the Prepared CDs
From the B-CDs and Y-CDs to R-CDs solution, the full width at half maximum (FWMH) was gradually decreased from 145 nm and 122 nm to 107 nm. Here, R-CDs possess a narrow FWMH, indicating the narrow band gap, which brought about the red emission.
We also optimized the reaction temperature (160, 180, 200 • C), reaction time (8, 10, 12, 14 h), and material ratio of o-phenylenediamin/1,8-diaminonaphthalene (1:2, 1:1, 2:1) at the pre-synthesis stage in order to obtain better fluorescence behavior. The fluorescence emission intensity of the R-CDs was investigated under these different conditions, and the results are shown in Figure S3. The optimal reaction conditions were a reaction temperature of180 • C, a reaction time of 12 h, and material ratio of o-phenylenediamin/1,8diaminonaphthalene = 1:1.
For comparison, the original UV-vis and fluorescence emission spectra of o-phenylenediamine, aniline, 1,8-diaminonaphthalene, and [1,1 -binaphthalene]-2,2 -diamine. are presented in Figure S4. These four raw molecules had a very slight blue emission, and the absorptions in the UV-vis spectra were all in the UV range of 200-400 nm, which differed from the prepared MCDs; this verified that new luminescent centers were formed in the MCDs.
As the emission wavelength of B-, Y-, and R-CDs shifted from 440 nm, 530 nm to 580 nm, the size of the CDs slightly increased from 1.97 nm to 2.51 nm. Here, the redshift of the emission wavelength had a positive correlation with the size of the CDs [30]. This phenomenon suggested that maybe the increased effective conjugation length, the high extent of graphitization, and the extended sp 2 domain gave rise to the increasing size.
To further comprehend the photoluminescence, the fluorescence lifetime decay curves of the blue, green, and red CDs were measured at 375 nm using a multi-dimensional timedependent single photon counting (TCSPC) method; the corresponding fitted equations with satisfactory goodness are shown in the supporting information. Using this method, the calculated average lifetimes (τ) were 5.08, 5.17 and 5.65 ns ( Figure S5). In addition, it was found that the two radiative lifetimes τ1 and τ2 could be ascribed to the intrinsic recombination of the carbon core states and surface states [1]. Here, we can observe that the ratio of τ2 increased gradually with the redshift in the emission wavelength (Table S2), which indicated the existence of enhanced surface states. The relative quantum yield was measured by using Rhodamine B as a reference. The calculated QY of the B-CDs, Y-CDs, and R-CDs were 33%, 59%, and 11%, respectively. Here, the relative fluorescence quantum yield and fluorescence lifetimes were comparable with those reported for multicolor CDs, showing their excellent optical properties. In addition, we suggest that the non-radiative transition centers lead to the relatively low QY of R-CDs.
The photostability of the MCDs was also discussed. From Figure S6, we can see that the fluorescence intensity of the MCDs remained basically unchanged after continuous irradiation for 7200 s, showing their outstanding photostability and anti-photobleaching capabilities. Meanwhile, the appearance and fluorescence property of the CDs solution showed no obvious change after storage at room temperature for 3 months.
The energy gaps of the B-, Y-, and R-CDs were calculated using the formula E gopt = 1240/λ edge , in which λ edge is the maximum absorption edge wavelength. The HOMO-LUMO energy gaps of the B-, Y-, and R-CDs ( Figure 6) were calculated as 3.19, 2.55, and 2.05 eV, respectively, corresponding to the redshift in the emission wavelength. This result was in accordance with the increase in the graphitic-N content. Based on the above results, the redshift in the CDs emission was attributed to the increase of the graphite N content in the carbon core and the oxidation degree on the sur face of the CDs.

The Applications of MCDs
The prepared three CDs displayed hydrophilicity, the ability to be easily dissolved in various kinds of polarity organic solvents, such as DMSO, DMF, and dichloromethane slight solubility in ethanol, but limited solubility in nonpolar organic solvents.
Several kinds of polymers can be used as solid-state luminescence matrices, such a poly-acrylic (PAA), poly-dimethylsiloxane (PDMS), and poly-vinylpyrrolidone (PVP) Considering that polyvinylpyrrolidone (PVA) has the advantages of a pure surface con formation, low cost, environmental friendliness, and good hydrophilicity, it was selected as the matrix to be used to fabricate CDs/PVA film. The B-CDs/PVA, Y-CDs/PVA, and R CDs/PVA films exhibited bright blue, yellow, and red emissions under UV light irradia tion, where aggregation and solid-state quenching can be effectively avoided. As shown in Figure SX, RCDs were well dispersed in the PVA matrix, and no obvious aggregation could be observed, thus proving that the PVA can be effective in preventing aggregation and fluorescence quenching of CDs. The fluorescence emission spectra of CDs/PVA film under the optimal excitation wavelength were depicted in Figure 7a. The optimal emission wavelengths were located at ≈440, ≈530, and ≈580 nm, respectively, which were the same wavelengths as the CDs in the solvents; this further confirms that the prepared CDs were homogeneously distributed in the PVA matrix with invariance property. The FWMHs o the B-CDs/PVA, Y-CDs/PVA, and R-CDs/PVA films were 111 nm, 104 nm, 85 nm, respec tively, which were much lower than those of the CDs solution, indicating their potentia to be applied in high color-purity displays and solid-state luminescence.
To further explore their practicability, the CDs/PVA films were used to package the LED chips. The CDs/PVA films were coated on UV chips to form illumination devices These MCDs-based LEDs produced bright monochrome blue, yellow, and red light (Fig  ure 8b), and the corresponding CIE coordinates were (0.16, 0.02), (0.38, 0.58), and (0.50 0.49), based on the emission spectra of the device (Figure 8a). These CDs-based LEDs show great potential in the multicolor lighting field. Based on the above results, the redshift in the CDs emission was attributed to the increase of the graphite N content in the carbon core and the oxidation degree on the surface of the CDs.

The Applications of MCDs
The prepared three CDs displayed hydrophilicity, the ability to be easily dissolved in various kinds of polarity organic solvents, such as DMSO, DMF, and dichloromethane, slight solubility in ethanol, but limited solubility in nonpolar organic solvents.
Several kinds of polymers can be used as solid-state luminescence matrices, such as poly-acrylic (PAA), poly-dimethylsiloxane (PDMS), and poly-vinylpyrrolidone (PVP). Considering that polyvinylpyrrolidone (PVA) has the advantages of a pure surface conformation, low cost, environmental friendliness, and good hydrophilicity, it was selected as the matrix to be used to fabricate CDs/PVA film. The B-CDs/PVA, Y-CDs/PVA, and R-CDs/PVA films exhibited bright blue, yellow, and red emissions under UV light irradiation, where aggregation and solid-state quenching can be effectively avoided. As shown in Figure S7, RCDs were well dispersed in the PVA matrix, and no obvious aggregation could be observed, thus proving that the PVA can be effective in preventing aggregation and fluorescence quenching of CDs. The fluorescence emission spectra of CDs/PVA films under the optimal excitation wavelength were depicted in Figure 7a. The optimal emission wavelengths were located at ≈440, ≈530, and ≈580 nm, respectively, which were the same wavelengths as the CDs in the solvents; this further confirms that the prepared CDs were homogeneously distributed in the PVA matrix with invariance property. The FWMHs of the B-CDs/PVA, Y-CDs/PVA, and R-CDs/PVA films were 111 nm, 104 nm, 85 nm, respectively, which were much lower than those of the CDs solution, indicating their potential to be applied in high color-purity displays and solid-state luminescence. Based on the above results, the redshift in the CDs emission was attributed to the increase of the graphite N content in the carbon core and the oxidation degree on the surface of the CDs.

The Applications of MCDs
The prepared three CDs displayed hydrophilicity, the ability to be easily dissolved in various kinds of polarity organic solvents, such as DMSO, DMF, and dichloromethane, slight solubility in ethanol, but limited solubility in nonpolar organic solvents.
Several kinds of polymers can be used as solid-state luminescence matrices, such as poly-acrylic (PAA), poly-dimethylsiloxane (PDMS), and poly-vinylpyrrolidone (PVP). Considering that polyvinylpyrrolidone (PVA) has the advantages of a pure surface conformation, low cost, environmental friendliness, and good hydrophilicity, it was selected as the matrix to be used to fabricate CDs/PVA film. The B-CDs/PVA, Y-CDs/PVA, and R-CDs/PVA films exhibited bright blue, yellow, and red emissions under UV light irradiation, where aggregation and solid-state quenching can be effectively avoided. As shown in Figure SX, RCDs were well dispersed in the PVA matrix, and no obvious aggregation could be observed, thus proving that the PVA can be effective in preventing aggregation and fluorescence quenching of CDs. The fluorescence emission spectra of CDs/PVA films under the optimal excitation wavelength were depicted in Figure 7a. The optimal emission wavelengths were located at ≈440, ≈530, and ≈580 nm, respectively, which were the same wavelengths as the CDs in the solvents; this further confirms that the prepared CDs were homogeneously distributed in the PVA matrix with invariance property. The FWMHs of the B-CDs/PVA, Y-CDs/PVA, and R-CDs/PVA films were 111 nm, 104 nm, 85 nm, respectively, which were much lower than those of the CDs solution, indicating their potential to be applied in high color-purity displays and solid-state luminescence.
To further explore their practicability, the CDs/PVA films were used to package the LED chips. The CDs/PVA films were coated on UV chips to form illumination devices. These MCDs-based LEDs produced bright monochrome blue, yellow, and red light (Figure 8b), and the corresponding CIE coordinates were (0.16, 0.02), (0.38, 0.58), and (0.50, 0.49), based on the emission spectra of the device (Figure 8a). These CDs-based LEDs show great potential in the multicolor lighting field. To further explore their practicability, the CDs/PVA films were used to package the LED chips. The CDs/PVA films were coated on UV chips to form illumination de-vices. These MCDs-based LEDs produced bright monochrome blue, yellow, and red light (Figure 8b), and the corresponding CIE coordinates were (0.16, 0.02), (0.38, 0.58), and (0.50, 0.49), based on the emission spectra of the device (Figure 8a). These CDs-based LEDs show great potential in the multicolor lighting field.

Characterizations
The size and morphology of the prepared MCDs were characterized by high-resolution transmission electron microscopy (TEM, JEOL JEM 2100F, Tokyo, Japan). The phase of the MCDs was characterized between 0° and 90° using 2θ scanning X-ray diffraction (XRD, Rigaku, Smart Lab 3KW, Japan). Fourier-transform infrared (FTIR) spectra were obtained on a spectrometer detector (Thermo, Nicolet is50, Madison, WI, USA). Raman spectra were measured on a confocal micro-Raman spectrometer detector (Thermo, DXR2, Madison, WI, USA). The MCDs prepared by the PHI1600EXCA photoelectron spectrometer were analyzed using X-ray photoelectron spectroscopy (Perkin-Elmer, USA). The ultraviolet-visible (UV-vis) absorption spectra of MCDs were implemented on a spectrophotometer (Purkinje, T9, Beijing, China). The fluorescence excitation/emission spectra of the MCDs were assembled using a fluorescence spectrophotometer (Hitachi, F-7000, Japan). The fluorescence decay curves were recorded on an FLS 1000 fluorescence spectrometer (Edinburgh Instruments, Livingston, UK).

Synthesis of CDs
As shown in Scheme 1, MCDs were composited using a simple solvothermal method. According to the procedure typically used to prepare R-CDs, o-phenylenediamine (0.25 mmol) and 1,8-diamino-naphthalene (0.25 mmol) were added to 10 mL of DMF. Then, the mixed solution was moved to a 100 mL Teflon-lined stainless-steel autoclave for a solvothermal pyrolysis reaction and heated at 180 °C for 12 h. After that, the autoclave was naturally chilled down to normal atmospheric temperature. Subsequently, the obtained MCD solution was dialyzed for 24 h through a 1000 Da dialysis membrane (molecular weight cutoff value) with ultrapure water to remove small molecules and unreacted chemical substances. Finally, the pure CD solution was kept at room temperature for further use. The purified CD solution was freeze-dried to obtain the CD dry powder, which was

Characterizations
The size and morphology of the prepared MCDs were characterized by high-resolution transmission electron microscopy (TEM, JEOL JEM 2100F, Tokyo, Japan). The phase of the MCDs was characterized between 0 • and 90 • using 2θ scanning X-ray diffraction (XRD, Rigaku, Smart Lab 3KW, Japan). Fourier-transform infrared (FTIR) spectra were obtained on a spectrometer detector (Thermo, Nicolet is50, Madison, WI, USA). Raman spectra were measured on a confocal micro-Raman spectrometer detector (Thermo, DXR2, Madison, WI, USA). The MCDs prepared by the PHI1600EXCA photoelectron spectrometer were analyzed using X-ray photoelectron spectroscopy (Perkin-Elmer, USA). The ultraviolet-visible (UV-vis) absorption spectra of MCDs were implemented on a spectrophotometer (Purkinje, T9, Beijing, China). The fluorescence excitation/emission spectra of the MCDs were assembled using a fluorescence spectrophotometer (Hitachi, F-7000, Japan). The fluorescence decay curves were recorded on an FLS 1000 fluorescence spectrometer (Edinburgh Instruments, Livingston, UK).

Synthesis of CDs
As shown in Scheme 1, MCDs were composited using a simple solvothermal method. According to the procedure typically used to prepare R-CDs, o-phenylenediamine (0.25 mmol) and 1,8-diamino-naphthalene (0.25 mmol) were added to 10 mL of DMF. Then, the mixed solution was moved to a 100 mL Teflon-lined stainless-steel autoclave for a solvothermal pyrolysis reaction and heated at 180 • C for 12 h. After that, the autoclave was naturally chilled down to normal atmospheric temperature. Subsequently, the obtained MCD solution was dialyzed for 24 h through a 1000 Da dialysis membrane (molecular weight cutoff value) with ultrapure water to remove small molecules and unreacted chemical substances. Finally, the pure CD solution was kept at room temperature for further use. The purified Molecules 2023, 28, 2957 9 of 12 CD solution was freeze-dried to obtain the CD dry powder, which was then ground and crushed into CD powder and characterized using XRD, FTIR and XPS.Y-CDs (precursor: 0.25 mmol o-phenylenediamine and 0.25 mmol aniline) and B-CDs (precursor: 0.25 mmol o-phenylenediamine and 0.25 mmol 1,1 -binaphthalene-2,2 -diamine) were obtained in the same way.

The Determination of the Relative Fluorescence Quantum Yield and Fluorescence L
The relative fluorescence quantum yield of B-CDs, Y-CD, and R-CDs were m by using Rhodamine B (QYstd: 89%) as a reference.
The QY can be calculated as follows: where "QY" is the quantum yield, "A" is the absorbance at the maximum e wavelength, "Ι" represents the fluorescence integral area at the maximum e wavelength, "η" is the refractive index of the solvent, and the subscripts "std" indicate the reference substance and the substance to be measured, respectively. T the impact of reabsorption, the absorbance of the measured substance at the m excitation wavelength was less than 0.05.
The fluorescence lifetime decay curves of B-CDs, Y-CDs, and R-CDs were m at 375 nm excitation using a multi-dimensional time-dependent single photon c (TCSPC) method, and the corresponding fitted equations and the calculated ave time (τ) equations are shown in the supporting information.

Preparation of CDs/PVA Films
In total, 4 g of PVA was dissolved in 16 mL of DMSO at 90 °C for 2 h in order a 20% PVA solution. Then, 10 mg of blue, yellow, and red luminous CD pow added to each 20% PVA solution (20 mL) while the mixture was constantly sti

The Determination of the Relative Fluorescence Quantum Yield and Fluorescence Lifetime
The relative fluorescence quantum yield of B-CDs, Y-CD, and R-CDs were measured by using Rhodamine B (QYstd: 89%) as a reference.
The QY can be calculated as follows: where "QY" is the quantum yield, "A" is the absorbance at the maximum excitation wavelength, "I" represents the fluorescence integral area at the maximum excitation wavelength, "η" is the refractive index of the solvent, and the subscripts "std" and "x" indicate the reference substance and the substance to be measured, respectively. To reduce the impact of reabsorption, the absorbance of the measured substance at the maximum excitation wavelength was less than 0.05. The fluorescence lifetime decay curves of B-CDs, Y-CDs, and R-CDs were measured at 375 nm excitation using a multi-dimensional time-dependent single photon counting (TCSPC) method, and the corresponding fitted equations and the calculated average lifetime (τ) equations are shown in the supporting information.

Preparation of CDs/PVA Films
In total, 4 g of PVA was dissolved in 16 mL of DMSO at 90 • C for 2 h in order to obtain a 20% PVA solution. Then, 10 mg of blue, yellow, and red luminous CD powder was added to each 20% PVA solution (20 mL) while the mixture was constantly stirred. The above solution was added to a self-made framework and naturally dried at room temperature for 24 h in order to obtain homogeneous CD/PVA films.

The Fabrication of CDs/PVA Composites-Based LEDs
Commercially available LED chips (emission centers at 365 nm) with no phosphorus coating were purchased from Advanced Optoelectronics Technology Inc. Then, the blue luminous CD/PVA film was fastened to the top of the LED chip in order to manufacture the blue LED. Yellow LEDs and red LEDs were also prepared by using the above method.

Conclusions
In summary, a new and simple synthetic procedure for preparing blue, yellow, and red emissive CDs was developed through the solvothermal method by using ophenylenediamine with aniline, 1,8-diaminonaphthalene and [1,1 -binaphthalene]-2,2diamine as precursors, respectively. The emission properties of the CDs can be tuned by choosing carbon precursors with different amounts of benzene rings. Related characterizations demonstrated that the redshift of CDs was ascribed to the increasing effective conjugation degree, the high graphitization degree, and size. The prepared MCDs can be dissolved well in the polarity organic solvents, forming homogeneous solutions with bright blue, yellow and red emissions. A PVA polymer was used as the matrix for the fabrication of the CDs/PVA films. The films exhibited bright blue, yellow, and red emissions under UV light, as is also exhibited in organic solvents that effectively avoid aggregation and fluorescence quenching. By deposing these CDs/PVA films on UV chips, blue, yellow, and red LED devices with the CIE coordinates of (0.16, 0.02), (0.38, 0.58), and (0.50, 0.49) were successfully fabricated. Multicolor LEDs were constructed in order to demonstrate their potential applications in solid-state luminescence.
Author Contributions: Z.L.: Conceptualization, methodology, validation, investigation, data curation, writing-original draft preparation; X.L.: Conceptualization, methodology; M.L.: Investigation, resources; W.W.: Writing-original draft preparation, writing-review and editing, supervision, project administration, funding acquisition. All authors have read and agreed to the published version of the manuscript.